Optimized scale factor for frequency band extension in an audio frequency signal decoder

ABSTRACT

A method and device are provided for determining an optimized scale factor to be applied to an excitation signal or a filter during a process for frequency band extension of an audio frequency signal. The band extension process includes decoding or extracting, in a first frequency band, an excitation signal and parameters of the first frequency band including coefficients of a linear prediction filter, generating an excitation signal extending over at least one second frequency band, filtering using a linear prediction filter for the second frequency band. The determination method includes determining an additional linear prediction filter, of a lower order than that of the linear prediction filter of the first frequency band, the coefficients of the additional filter being obtained from the parameters decoded or extracted from the first frequency band and calculating the optimized scale factor as a function of at least the coefficients of the additional filter.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a Section 371 National Stage Application ofInternational Application No. PCTFR2014/051720, filed Jul. 4, 2014, thecontent of which is incorporated herein by reference in its entirety,and published as WO 2015/004373 on Jan. 15, 2015, not in English.

FIELD OF THE DISCLOSURE

The present invention relates to the field of the coding/decoding andthe processing of audio frequency signals (such as speech, music orother such signals) for their transmission or their storage.

More particularly, the invention relates to a method and a device fordetermining an optimized scale factor that can be used to adjust thelevel of an excitation signal or, in an equivalent manner, of a filteras part of a frequency band extension in a decoder or a processorenhancing an audio frequency signal.

BACKGROUND OF THE DISCLOSURE

Numerous techniques exist for compressing (with loss) an audio frequencysignal such as speech or music.

The conventional coding methods for the conversational applications aregenerally classified as waveform coding (PCM for “Pulse CodeModulation”, ADCPM for “Adaptive Differential Pulse Code Modulation”,transform coding, etc.), parametric coding (LPC for “Linear PredictiveCoding”, sinusoidal coding, etc.) and parametric hybrid coding with aquantization of the parameters by “analysis by synthesis” of which CELP(“Code Excited Linear Prediction”) coding is the best known example.

For the non-conversational applications, the prior art for (mono) audiosignal coding consists of perceptual coding by transform or in subbands,with a parametric coding of the high frequencies by band replication.

A review of the conventional speech and audio coding methods can befound in the works by W. B. Kleijn and K. K. Paliwal (eds.), SpeechCoding and Synthesis, Elsevier, 1995; M. Bosi, R. E. Goldberg,Introduction to Digital Audio Coding and Standards, Springer 2002; J.Benesty, M. M. Sondhi, Y. Huang (Eds.), Handbook of Speech Processing,Springer 2008.

The focus here is more particularly on the 3GPP standardized AMR-WB(“Adaptive Multi-Rate Wideband”) codec (coder and decoder), whichoperates at an input/output frequency of 16 kHz and in which the signalis divided into two subbands, the low band (0-6.4 kHz) which is sampledat 12.8 kHz and coded by CELP model and the high band (6.4-7 kHz) whichis reconstructed parametrically by “band extension” (or BWE, for“Bandwidth Extension”) with or without additional information dependingon the mode of the current frame. It can be noted here that thelimitation of the coded band of the AMR-WB codec at 7 kHz is essentiallylinked to the fact that the frequency response in transmission of thewideband terminals was approximated at 3.0 the time of standardization(ETSI/3GPP then ITU-T) according to the frequency mask defined in thestandard ITU-T P.341 and more specifically by using a so-called “P341”filter defined in the standard ITU-T G.191 which cuts the frequenciesabove 7 kHz (this filter observes the mask defined in P.341). However,in theory, it is well known that a signal sampled at 16 kHz can have adefined audio band from 0 to 8000 Hz; the AMR-WB codec thereforeintroduces a limitation of the high band by comparison with thetheoretical bandwidth of 8 kHz.

The 3GPP AMR-WB speech codec was standardized in 2001 mainly for thecircuit mode (CS) telephony applications on GSM (2G) and UMTS (3G). Thissame codec was also standardized in 2003 by the ITU-T in the form ofrecommendation G.722.2 “Wideband coding speech at around 16 kbit/s usingAdaptive Multi-Rate Wideband (AMR-WB)”.

It comprises nine bit rates, called modes, from 6.6 to 23.85 kbit/s, andcomprises continuous transmission mechanisms (DTX, for “DiscontinuousTransmission”) with voice activity detection (VAD) and comfort noisegeneration (CNG) from silence description frames (SID, for “SilenceInsertion Descriptor”), and lost frame correction mechanisms (FEC for“Frame Erasure Concealment”, sometimes called PLC, for “Packet LossConcealment”).

The details of the AMR-WB coding and decoding algorithm are not repeatedhere; a detailed description of this codec can be found in the 3GPPspecifications (TS 26.190, 26.191, 26.192, 26.193, 26.194, 26.204) andin ITU-T-G.722.2 (and the corresponding annexes and appendix) and in thearticle by B. Bessette et al. entitled “The adaptive multirate widebandspeech codec (AMR-WB)”, IEEE Transactions on Speech and AudioProcessing, vol. 10, no. 8, 2002, pp. 620-636 and the source code of theassociated 3GPP and ITU-T standards.

The principle of band extension in the AMR-WB codec is fairlyrudimentary. Indeed, the high band (6.4-7 kHz) is generated by shaping awhite noise through a time (applied in the form of gains per subframe)and frequency (by the application of a linear prediction synthesisfilter or LPC, for “Linear Predictive Coding”) envelope. This bandextension technique is illustrated in FIG. 1.

A white noise u_(HB1)(n), n=0, . . . , 79 is generated at 16 kHz foreach 5 ms subframe by linear congruential generator (block 100). Thisnoise u_(HB1)(n) is formatted in time by application of gains for eachsubframe; this operation is broken down into two processing steps(blocks 102, 106 or 109):

-   -   A first factor is computed (block 101) to set the white noise        u_(HB1)(n) (block 102) at a level similar to that of the        excitation, u(n), n=0, . . . , 63, decoded at 12.8 kHz in the        low band:

${u_{{HB}\; 2}(n)} = {{u_{{HB}\; 1}(n)}\sqrt{\frac{\sum\limits_{t = 0}^{63}\; {u(l)}^{2}}{\sum\limits_{t = 0}^{79}\; {u_{{HB}\; 1}(l)}^{2}}}}$

It can be noted here that the normalization of the energies is done bycomparing blocks of different size (64 for u(n) and 80 for u_(HB1)(n))without compensation of the differences in sampling frequencies (12.8 or16 kHz).

The excitation in the high band is then obtained (block 106 or 109) inthe form:

u _(HB)(n)=ĝ _(HB) u _(HB2)(n)

-   -   in which the gain ĝ_(HB) is obtained differently depending on        the bit rate. If the bit rate of the current frame is <23.85        kbit/s, the gain ĝ_(HB) is estimated “blind” (that is to say        without additional information); in this case, the block 103        filters the signal decoded in low band by a high-pass filter        having a cut-off frequency at 400 Hz to obtain a signal        ŝ_(hp)(n), n=0, . . . , 63—this high-pass filter eliminates the        influence of the very low frequencies which can skew the        estimation made in the block 104 then the “tilt” (indicator of        spectral slope) denoted e_(tilt) of the signal ŝ_(hp) (n) is        computed by normalized self-correlation (block 104):

$e_{tilt} = \frac{\sum\limits_{n = 1}^{63}\; {{{\hat{s}}_{hp}(n)}{{\hat{s}}_{hp}\left( {n - 1} \right)}}}{\sum\limits_{n = 0}^{63}\; {{\hat{s}}_{hp}(n)}^{2}}$

-   -   and finally, ĝ_(HB) is computed in the form:

ĝ _(HB) =w _(SP) g _(SP)+(1−w _(SP))g _(BG)

-   -   in which g_(SP)=1−e_(tilt) is the gain applied in the active        speech (SP) frames, g_(BG)=1.25g_(SP) is the gain applied in the        inactive speech frames associated with a background (BG) noise        and w_(SP) is a weighting function which depends on the voice        activity detection (VAD). It is understood that the estimation        of the tilt (e_(tilt)) makes it possible to adapt the level of        the high band as a function of the spectral nature of the        signal; this estimation is particularly important when the        spectral slope of the CELP decoded signal is such that the        average energy decreases when the frequency increases (case of a        voiced signal where e_(tilt) is close to 1, therefore        g_(SP)=1−e_(tilt) is thus reduced). It should also be noted that        the factor ĝ_(HB) in the AMR-WB decoding is bounded to take        values within the range [0.1, 1.0]. Indeed, for the signals        whose energy increases when the frequency increases (e_(tilt)        close to −1, g_(SP) close to 2), the gain ĝ_(HB) is usually        underestimated.

At 23.85 kbit/s, a correction information item is transmitted by theAMR-WB coder and decoded (blocks 107, 108) in order to refine the gainestimated for each subframe (4 bits every 5 ms, or 0.8 kbit/s). Theartificial excitation u_(HB)(n) is then filtered (block 111) by an LPCsynthesis filter (block 111) of transfer function 1/A_(HB)(z) andoperating at the sampling frequency of 16 kHz. The construction of thisfilter depends on the bit rate of the current frame:

-   -   At 6.6 kbit/s, the filter 1/A_(HB)(z) is obtained by weighting        by a factor γ=0.9 an LPC filter of order 20, 1/Â^(ext)(z) which        “extrapolates” the LPC filter of order 16, 1/Â(z), decoded in        the low band (at 12.8 kHz)—the details of the extrapolation in        the realm of the ISF (Imittance Spectral Frequency) parameters        are described in the standard G.722.2 in section 6.3.2.1; in        this case, 1/A_(HB)(z)=1/Â^(ext)(z/γ)    -   at the bit rates >6.6 kbit/s, the filter 1/A_(HB) (z) is of        order 16 and corresponds simply to:

1/A _(HB)(z)=1/Â(z/γ)

-   -   in which γ=0.6. It should be noted that, in this case, the        filter 1/Â(z/γ) is used at 16 kHz, which results in a spreading        (by proportional transformation) of the frequency response of        this filter from [0, 6.4 kHz] to [0, 8 kHz].

The result, s_(HB)(n), is finally processed by a bandpass filter (block112) of FIR (“Finite Impulse Response”) type, to keep only the 6-7 kHzband; at 23.85 kbit/s, a low-pass filter also of FIR type (block 113) isadded to the processing to further attenuate the frequencies above 7kHz. The high frequency (HF) synthesis is finally added (block 130) tothe low frequency (LF) synthesis obtained with the blocks 120 to 122 andre-sampled at 16 kHz (block 123). Thus, even 3.5 if the high bandextends in theory from 6.4 to 7 kHz in the AMR-WB codec, the HFsynthesis is rather contained in the 6-7 kHz band before addition withthe LF synthesis.

A number of drawbacks in the band extension technique of the AMR-WBcodec can be identified, in particular:

-   -   the estimation of gains for each subframe (block 101, 103 to        105) is not optimal. Partly, it is based on an equalization of        the “absolute” energy per subframe (block 101) between signals        at different frequencies: artificial excitation at 16 kHz (white        noise) and a signal at 12.8 kHz (decoded ACELP excitation). It        can be noted in particular that this approach implicitly induces        an attenuation of the high-band excitation (by a ratio        12.8/16=0.8); in fact, it will also be noted no de-emphasis is        performed on the high band in the AMR-WB codec, which implicitly        induces an amplification relatively close to 0.6 (which        corresponds to the value of the frequency response of        1/(1−0.68z⁻¹) at 6400 Hz). In fact, the factors of 1/0.8 and of        0.6 are compensated approximately.    -   Regarding speech, the 3GPP AMR-WB codec characterization tests        documented in the 3GPP report TR 26.976 have shown that the mode        at 23.85 kbit/s has a less good quality than at 23.05 kbit/s,        its quality being in fact similar to that of the mode at 15.85        kbit/s. This shows in particular that the level of artificial HF        signal has to be controlled very prudently, because the quality        is degraded at 23.85 kbit/s whereas the 4 bits per frame are        considered to best make it possible to approximate the energy of        the original high frequencies.    -   The low-pass filter at 7 kHz (block 113) introduces a shift of        almost 1 ms between the low and high bands, which can        potentially degrade the quality of certain signals by slightly        desynchronizing the two bands at 23.85 kbit/s this        desynchronization can also pose problems when switching bit rate        from 23.85 kbit/s to other modes.

An example of band extension via a temporal approach is described in the3GPP standard TS 26.290 describing the AMR-WB+ codec (standardized in2005). This example is illustrated in the block diagrams of FIGS. 2a(general block diagram) and 2 b (gain prediction by response levelcorrection) which correspond respectively to FIGS. 16 and 10 of the 3GPPspecification TS 26.290.

In the AMR-WB+ codec, the (mono) input signal sampled at the frequencyFs (in Hz) is divided into two separate frequency bands, in which twoLPC filters are computed and coded separately:

-   -   one LPC filter, denoted A(z), in the low band (0−Fs/4)—its        quantized version is denoted Â(z)    -   another LPC filter, denoted A_(HF) (Z), in the spectrally        aliased high band (Fs/4−Fs/2)—its quantized version is denoted        Â_(HF)(z)

The band extension is done in the AMR-WB+ codec as detailed in sections5.4 (HF coding) and 6.2 (HF decoding) of the 3GPP specification TS26.290. The principle thereof is summarized here: the extension consistsin using the excitation decoded at low frequencies (LFC excit.) and informatting this excitation by a temporal gain per subframe (block 205)and an LPC synthesis filtering (block 207); the processing operations toenhance (post-processing) the excitation (block 206) and smooth theenergy of the reconstructed HF signal (block 208) are moreoverimplemented as illustrated in FIG. 2 a.

It is important to note that this extension in AMR-WB+ necessitates thetransmission of additional information: the coefficients of the filterÂ_(HF)(z) in 204 and a temporal formatting gain per subframe (block201). One particular feature of the band extension algorithm in AMR-WB+is that the gain per subframe is quantified by a predictive approach; inother words, the gains are not coded directly, but rather gaincorrections which are relative to an estimation of the gain denotedg_(match). This estimation, g_(match), actually corresponds to a levelequalization factor between the filters Â(z) and Â_(HF)(z) at thefrequency of separation between low band and high band (Fs/4). Thecomputation of the factor g_(match) (block 203) is detailed in FIG. 10of the 3GPP specification TS 26.290 reproduced here in FIG. 2b . Thisfigure will not be detailed more here. It will simply be noted that theblocks 210 to 213 are used to compute the energy of the impulse responseof

$\frac{{\hat{A}}_{z}}{\left( {1 - {0.9z^{- 1}}} \right){{\hat{A}}_{HF}(z)}},$

while recalling that the filter Â_(HF)(z) models a spectrally aliasedhigh band (because of the spectral properties of the filter bankseparating the low and high bands). Since the filters are interpolatedby subframes, the gain g_(match) is computed only once per frame, and itis interpolated by subframes.

The band extension gain coding technique in AMR-WB+, and moreparticularly the compensation of levels of the LPC filters at theirjunction is an appropriate method in the context of a band extension byLPC models in low and high band, and it can be noted that such a levelcompensation between LPC filters is not present in the band extension ofthe AMR-WB codec. However, it is in practice possible to verify that thedirect equalization of the level between the two LPC filters at theseparation frequency is not an optimal method and can provoke anoverestimation of energy in high band and audible artifacts in certaincases; it will be recalled that an LPC filter represents a spectralenvelope, and the principle of equalization of the level between two LPCfilters for a given frequency amounts to adjusting the relative level oftwo LPC envelopes. Now, such an equalization performed at a precisefrequency does not ensure a complete continuity and overall consistencyof the energy (in frequency) in the vicinity of the equalization pointwhen the frequency envelope of the signal fluctuates significantly inthis vicinity. A mathematical way of positing the problem consists innoting that the continuity between two curves can be ensured by forcingthem to meet at one and the same point, but there is nothing toguarantee that the local properties (successive derivatives) coincide soas to ensure a more global consistency. The risk in ensuring a spotcontinuity between low and high band LPC envelopes is of setting the LPCenvelope in high band at a relative level that is too strong or tooweak, the case of a level that is too strong being more damaging becauseit results in more annoying artifacts.

Moreover, the gain compensation in AMR-WB+ is primarily a prediction ofthe gain known to the coder and to the decoder and which serves toreduce the bit rate necessary for the transmission of gain informationscaling the high-band excitation signal. Now, in the context of aninteroperable enhancement of the AMR-WB coding/decoding, it is notpossible to modify the existing coding of the gains by subframes (0.8kbit/s) of the band extension in the AMR-WB 23.85 kbit/s mode.Furthermore, for the bit rates strictly less than 23.85 kbit/s, thecompensation of levels of LPC filters in low and high bands can beapplied in the band extension of a decoding compatible with AMR-WB, butexperience shows that this sole technique derived from the AMR-WB+coding, applied without optimization, can cause problems ofoverestimation of energy of 3.0 the high band (>6 kHz).

There is therefore a need to improve the compensation of gains betweenlinear prediction filters of different frequency bands for the frequencyband extension in a codec of AMR-WB type or an interoperable version ofthis codec without in any way overestimating the energy in a frequencyband and without requiring additional information from the coder.

SUMMARY

The present invention improves the situation.

To this end, the invention targets a method for determining an optimizedscale factor to be applied to an excitation signal or to a filter in anaudio frequency signal frequency band extension method, the bandextension method comprising a step of decoding or of extraction, in afirst frequency band, of an excitation signal and of parameters of thefirst frequency band comprising coefficients of a linear predictionfilter, a step of generation of an extended excitation signal on atleast one second frequency band and a step of filtering, by a linearprediction filter, for the second frequency band. The determinationmethod is such that it comprises the following steps:

-   -   determination of a linear prediction filter called additional        filter, of lower order than the linear prediction filter of the        first frequency band, the coefficients of the additional filter        being obtained from the parameters decoded or extracted from the        first frequency band; and    -   computation of the optimized scale factor as a function at least        of the coefficients of the additional filter.

Thus, the use of an additional filter of lower order than the filter ofthe first frequency band to be equalized makes it possible to avoid theoverestimations of energy in the high frequencies which could resultfrom local fluctuations of the envelope and which can disrupt theequalization of the prediction filters.

The equalization of gains between the linear prediction filters of thefirst and second frequency bands is thus enhanced.

In an advantageous application of the duly obtained optimized scalefactor, the band extension method comprises a step of application of theoptimized scale factor to the extended excitation signal.

In an appropriate embodiment, the application of the optimized scalefactor is combined with the step of filtering in the second frequencyband.

Thus, the steps of filtering and of application of the optimized scalefactor are combined in a single filtering step to reduce the processingcomplexity.

In a particular embodiment, the coefficients of the additional filterare obtained by truncation of the transfer function of the linearprediction filter of the first frequency band to obtain a lower order.

This lower order additional filter is therefore obtained in a simplemanner.

Furthermore, so as to obtain a stable filter, the coefficients of theadditional filter are modified as a function of a stability criterion ofthe additional filter.

In a particular embodiment, the computation of the optimized scalefactor comprises the following steps:

-   -   computation of the frequency responses of the linear prediction        filters of the first and second frequency bands for a common        frequency;    -   computation of the frequency response of the additional filter        for this common frequency;    -   computation of the optimized scale factor as a function of the        duly computed frequency responses.

Thus, the optimized scale factor is computed in such a way as to avoidthe annoying artifacts which could occur should the higher order filterfrequency response of the first band in proximity to the commonfrequency show a signal peak or trough.

In a particular embodiment, the method further comprises the followingsteps, implemented for a predetermined decoding bit rate:

-   -   first scaling of the extended excitation signal by a gain        computed per subframe as a function of an energy ratio between        the decoded excitation signal and the extended excitation        signal;    -   second scaling of the excitation signal obtained from the first        scaling by a decoded correction gain;    -   adjustment of the energy of the excitation for the current        subframe by an adjustment factor computed as a function of the        energy of the signal obtained after the second scaling and as a        function of the signal obtained after application of the        optimized scale factor.

Thus, additional information can be used to enhance the quality of theextended signal for a predetermined operating mode.

The invention also targets a device for determining an optimized scalefactor to be applied to an excitation signal or to a filter in an audiofrequency signal frequency band extension device, the band extensiondevice comprising a module for decoding or extracting, in a firstfrequency band, an excitation signal and parameters of the firstfrequency band comprising coefficients of a linear prediction filter, amodule for generating an extended excitation signal on at least onesecond frequency band and a module for filtering, by a linear predictionfilter, for the second frequency band. The determination device is suchthat it comprises:

-   -   a module for determining a linear prediction filter called        additional filter, of lower order than the linear prediction        filter of the first frequency band, the coefficients of the        additional filter being obtained from the parameters decoded or        extracted from the first frequency band; and    -   a module for computing the optimized scale factor as a function        at least of the coefficients of the additional filter.

The invention targets a decoder comprising a device as described.

It targets a computer program comprising code instructions forimplementing the steps of the method for determining an optimized scalefactor as described, when these instructions are executed by aprocessor.

Finally, the invention relates to a storage medium, that can be read bya processor, incorporated or not in the device for determining anoptimized scale factor, possibly removable, storing a computer programimplementing a method for determining an optimized scale factor asdescribed previously.

BRIEF DESCRIPTION OF THE DRAWINGS

Other features and advantages of the invention will become more clearlyapparent on reading the following description, given purely as anonlimiting example and with reference to the attached drawings, inwhich:

FIG. 1 illustrates a part of a decoder of AMR-WB type implementingfrequency band extension steps of the prior art and as describedpreviously;

FIGS. 2a and 2b present the coding of the high band in the AMR-WB+ codecaccording to the prior art and as described previously;

FIG. 3 illustrates a decoder that can interwork with the AMR-WB coding,incorporating a band extension device used according to an embodiment ofthe invention;

FIG. 4 illustrates a device for determining a scale factor optimized bya subframe as a function of the bit rate, according to an embodiment ofthe invention; and

FIGS. 5a and 5b illustrate the frequency responses of the filters usedfor the computation of the optimized scale factor according to anembodiment of the invention;

FIG. 6 illustrates, in flow diagram form, the main steps of a method fordetermining an optimized scale factor according to an embodiment of theinvention;

FIG. 7 illustrates an embodiment in the frequency domain of a device fordetermining an optimized scale factor as part of a band extension;

FIG. 8 illustrates a hardware implementation of an optimized scalefactor determination device in a band extension according to theinvention.

DETAILED DESCRIPTION OF ILLUSTRATIVE EMBODIMENTS

FIG. 3 illustrates an exemplary decoder, compatible with theAMR-WB/G.722.2 standard in which there is a band extension comprising adetermination of an optimized scale factor according to an embodiment ofthe method of the invention, implemented by the band extension deviceillustrated by the block 309.

Unlike the AMR-WB decoding which operates with an output samplingfrequency of 16 kHz, a decoder is considered here which can operate withan output signal (synthesis) at the frequency fs=8, 16, 32 or 48 kHz. Itshould be noted that it is assumed here that the coding has beenperformed according to the AMR-WB algorithm with an internal frequencyof 12.8 kHz for the CELP coding in low band and at 23.85 kbit/s with again coding per subframe at the frequency of 16 kHz; even though theinvention is described here at the decoding level, it is assumed herethat the coding can also operate with an input signal at the frequencyfs=8, 16, 32 or 48 kHz and suitable resampling operations, beyond thecontext of the invention, are implemented in coding as a function of thevalue of fs. It can be noted that, when fs=8 kHz, in the case of adecoding compatible with AMR-WB, it is not necessary to extend the 0-6.4kHz low band, because the audio band reconstructed at the frequency fsis limited to 0-4000 Hz.

In FIG. 3, the CELP decoding (LF for low frequencies) still operates atthe internal frequency of 12.8 kHz, as in AMR-WB, and the band extension(HF for high frequencies) used for the invention operates at thefrequency of 16 kHz, and the LF and HF syntheses are combined (block312) at the frequency fs after suitable resampling (block 306 andinternal processing in the block 311). In the variant embodiments, thecombining of the low and high bands can be done at 16 kHz, after havingresampled the low band from 12.8 to 16 kHz, before resampling thecombined signal at the frequency fs.

The decoding according to FIG. 3 depends on the AMR-WB mode (or bitrate) associated with the current frame received. As an indication, andwithout affecting the block 309, the decoding of the CELP part in lowband comprises the following steps:

-   -   demultiplexing of the coded parameters (block 300) in the case        of a frame correctly received (bfi=0 where bfi is the “bad frame        indicator” with a value 0 for a frame received and 1 for a frame        lost);    -   decoding of the ISF parameters with interpolation and conversion        into LPC coefficients (block 301) as described in clause 6.1 of        the standard G.722.2;    -   decoding of the CELP excitation (block 302), with an adaptive        and fixed part for reconstructing the excitation (exc or u′(n))        in each subframe of length 64 at 12.8 kHz:

u′(n)=ĝ _(p) v+ĝ _(c) c(n),n=0, . . . ,63

-   -   by following the notations of clause 7.1.2.1 of ITU-T        recommendation G.718 of a decoder interoperable with the AMR-WB        coder/decoder, concerning the CELP decoding, where v(n) and c(n)        are respectively the code words of the adaptive and fixed        dictionaries, and ĝ_(p) and ĝ_(c) are the associated decoded        gains. This excitation u′(n) is used in the adaptive dictionary        of the next subframe; it is then post-processed and, as in        G.718, the excitation u′(n) (also denoted exc) is distinguished        from its modified post-processed version u(n) (also denoted        exc2) which serves as input for the synthesis filter, 1/Â(z), in        the block 303;    -   synthesis filtering by 1/Â(z) (block 303) where the decoded LPC        filter Â(z) is of the order 16;    -   narrow-band post-processing (block 304) according to clause 7.3        of G.718 if fs=8 kHz;    -   de-emphasis (block 305) by the filter 1/(1−0.68z⁻¹);    -   post-processing of the low frequencies (called “bass posfilter”)        (block 306) attenuating the cross-harmonics noise at low        frequencies as described in clause 7.14.1.1 of G.718. This        processing introduces a delay which is taken into account in the        decoding of the high band (>6.4 kHz);    -   resampling of the internal frequency of 12.8 kHz at the output        frequency fs (block 307). A number of embodiments are possible.        Without losing generality, it is considered here, by way of        example, that if fs=8 or 16 kHz, the resampling described in        clause 7.6 of G.718 is repeated here, and if fs=32 or 48 kHz,        additional finite impulse response (FIR) filters are used;    -   computation of the parameters of the “noise gate” (block 308)        preferentially performed as described in clause 7.14.3 of G.718        to “enhance” the quality of the silences by level reduction.

In variants which can be implemented for the invention, thepost-processing operations applied to the excitation can be modified(for example, the phase dispersion can be enhanced) or thesepost-processing operations can be extended (for example, a reduction ofthe cross-harmonics noise can be implemented), without affecting thenature of the band extension.

It can be noted that the use of blocks 306, 308, 314 is optional.

It will also be noted that the decoding of the low band described aboveassumes a so-called “active” current frame with a bit rate between 6.6and 23.85 kbit/s. In fact, when the DTX mode is activated, certainframes can be coded as “inactive” and in this case it is possible toeither transmit a silence descriptor (on 35 bits) or transmit nothing.In particular, it will be recalled that the SID frame describes a numberof parameters: ISF parameters averaged over 8 frames, average energyover 8 frames, “dithering” flag for the reconstruction of non-stationarynoise. In all cases, in the decoder, there is the same decoding model asfor an active frame, with a reconstruction of the excitation and of anLPC filter for the current frame, which makes it possible to apply theband extension even to inactive frames. The same observation applies forthe decoding of “lost frames” (or FEC, PLC) in which the LPC model isapplied.

In the embodiment described here and with reference to FIG. 7, thedecoder makes it possible to extend the decoded low band (50-6400 Hztaking into account the 50 Hz high-pass filtering on the decoder, 0-6400Hz in the general case) to an extended band, the width of which varies,ranging approximately from 50-6900 Hz to 50-7700 Hz depending on themode implemented in the current frame. It is thus possible to refer to afirst frequency band of 0 to 6400 Hz and to a second frequency band of6400 to 8000 Hz. In reality, in the preferred embodiment, the extensionof the excitation is performed in the frequency domain in a 5000 to 8000Hz band, to allow a bandpass filtering of 6000 to 6900 or 7700 Hz width.

At 23.85 kbit/s, the HF gain correction information (0.8 kbit/s)transmitted at 23.85 kbit/s is here decoded. Its use is detailed later,with reference to FIG. 4. The high-band synthesis part is produced inthe block 309 representing the band extension device used for theinvention and which is detailed in FIG. 7 in an embodiment.

In order to align the decoded low and high bands, a delay (block 310) isintroduced to synchronize the outputs of the blocks 306 and 307 and thehigh band synthesized at 16 kHz is resampled from 16 kHz to thefrequency fs (output of block 311). The value of the delay T depends onhow the high band signal is synthesized, and on the frequency fs as inthe post-processing of the low frequencies. Thus, generally, the valueof Tin the block 310 will have to be adjusted according to the specificimplementation.

The low and high bands are then combined (added) in the block 312 andthe synthesis obtained is post-processed by 50 Hz high-pass filtering(of IIR type) of order 2, the coefficients of which depend on thefrequency fs (block 313) and output post-processing with optionalapplication of the “noise gate” in a manner similar to G.718 (block314).

Referring to FIG. 3, an embodiment of a device for determining anoptimized scale factor to be applied to an excitation signal in afrequency band extension process is now described. This device isincluded in the band extension block 309 described previously.

Thus, the block 400, from an excitation signal decoded in a firstfrequency band u(n), performs a band extension to obtain an extendedexcitation signal u_(HB)(n) on at least one second frequency band.

It will be noted here that the optimized scale factor estimationaccording to the invention is independent of how the signal u_(HB)(n) isobtained. One condition concerning its energy is, however, important.Indeed, the energy of the high band from 6000 to 8000 Hz must be at alevel similar to the energy of the band from 4000 to 6000 Hz of thedecoded excitation signal at the output of the block 302. Furthermore,since the low-band signal is de-emphasized (block 305), the de-emphasismust also be applied to the high-band excitation signal, either by usinga specific de-emphasis filter, or by multiplying by a constant factorwhich corresponds to an average attenuation of the filter mentioned.This condition does not apply to the case of the 23.85 kbit/s bit ratewhich uses the additional information transmitted by the coder. In thiscase, the energy of the high-band excitation signal must be consistentwith the energy of the signal corresponding to the coder, as explainedlater.

The frequency band extension can, for example, be implemented in thesame way as for the decoder of AMR-WB type described with reference toFIG. 1 in the blocks 100 to 102, from a white noise.

In another embodiment, this band extension can be performed from acombination of a white noise and of a decoded excitation signal asillustrated and described later for the blocks 700 to 707 in FIG. 7.

Other frequency band extension methods with conservation of the energylevel between the decoded excitation signal and the extended excitationsignal as described below, can of course be envisaged for the block 400.

Furthermore, the band extension module can also be independent of thedecoder and can perform a band extension for an existing audio signalstored or transmitted to the extension module, with an analysis of theaudio signal to extract an excitation and an LPC filter therefrom. Inthis case, the excitation signal at the input of the extension module isno longer a decoded signal but a signal extracted after analysis, likethe coefficients of the linear prediction filter of the first frequencyband used in the method for determining the optimized scale factor in animplementation of the invention.

In the example illustrated in FIG. 4, the case of the bit rates <23.85kbit/s, for which the determination of the optimized scale factor islimited to the block 401, is considered first. In this case, anoptimized scale factor denoted g_(HB2)(m) is computed. In oneembodiment, this computation is performed preferentially for eachsubframe and it consists in equalizing the levels of the frequencyresponses of the LPC filters 1/Â(z) and 1/Â(z/γ) used in low and highfrequencies, as described later with reference to FIG. 7, withadditional precautions to avoid the cases of overestimations which canresult in an excessive energy of the synthesized high band and thereforegenerate audible artifacts.

In an alternative embodiment, it will be possible to keep theextrapolated HF synthesis filter 1/Â^(ext)(z/γ) as implemented in theAMR-WB decoder or a decoder that can interwork with the AMR-WBcoder/decoder, for example according to the ITU-T recommendation G.718,in place of the filter 1/Â(z/γ). The compensation according to theinvention is then performed from the filters 1/Â(z) and 1/Â^(ext)(z/γ).

The determination of the optimized scale factor is also performed by thedetermination (in 401 a) of a linear prediction filter called additionalfilter, of lower order than the linear prediction filter of the firstfrequency band 1/Â(z), the coefficients of the additional filter beingobtained from the parameters decoded or extracted from the firstfrequency band. The optimized scale factor is then computed (in 401 b)as a function at least of these coefficients to be applied to theextended excitation signal u_(HB)(n).

The principle of the determination of the optimized scale factor,implemented in the block 401, is illustrated in FIGS. 5a and 5b withconcrete examples obtained from signals sampled at 16 kHz; the frequencyresponse amplitude values, denoted R, P, Q below, of 3 filters arecomputed at the common frequency of 6000 Hz (vertical dotted line) inthe current subframe, of which the index m is not recalled here in thenotations of the LPC filters interpolated by subframe to lighten thetext. The value of 6000 Hz is chosen such that it is close to theNyquist frequency of the low band, that is 6400 Hz. It is preferable notto take this Nyquist frequency to determine the optimized scale factor.Indeed, the energy of the decoded signal in low frequencies is typicallyalready attenuated at 6400 Hz. Furthermore, the band extension describedhere is performed on a second frequency band, called high band, whichranges from 6000 to 8000 Hz. It should be noted that, in variants of theinvention, a frequency other than 6000 Hz will be able to be chosen,with no loss of generality for determining the optimized scale factor.It will also be possible to consider the case where the two LPC filtersare defined for the separate bands (as in AMR-WB+). In this case, R, Pand Q will be computed at the separation frequency.

FIGS. 5a and 5b illustrate how the quantities R, P, Q are defined.

The first step consists in computing the frequency responses R and Prespectively of the linear prediction filter of the first frequency band(low band) and of the second frequency band (high band) at the frequencyof 6000 Hz. The following is first computed:

$R = {\frac{1}{{\hat{A}\left( ^{j\theta} \right)}} = \frac{1}{{\sum\limits_{i = 0}^{M}\; {{\hat{a}}_{i}^{j\theta}}}}}$

in which M=16 is the order of the decoded LPC filter, 1/Â(z), and θcorresponds to the frequency of 6000 Hz normalized for the samplingfrequency of 12.8 kHz, that is:

$\theta = {2\pi {\frac{6000}{12800}.}}$

Then, similarly, the following is computed:

$P = {\frac{1}{{\hat{A}\left( {^{{j\theta}^{\prime}}\text{/}\gamma} \right)}} = \frac{1}{{\sum\limits_{i = 0}^{M}\; {{\hat{a}}_{i}\gamma^{}^{- {j\theta}^{\prime}}}}}}$

in which

$\theta^{\prime} = {2\pi {\frac{6000}{16000}.}}$

In a preferred embodiment, the quantities P and R are computed accordingto the following pseudo-code:

  px = py = 0 rx = ry = 0 for i = 0 to 16  px = px + Ap[i]*exp_tab_p[i] py = py + Ap[i]*exp_tab_p[33-i]  rx = rx + Aq[i]*exp_tab_q[i]  ry = ry+Aq[i]*exp_tab_q[33-i] end for P = 1/sqrt(px*px + py*py) R =1/sqrt(rx*rx + ry*ry)in which Aq[i]=â_(i) corresponds to the coefficients of Â(z) (of order16), Ap[i]=γ^(i)â_(i) corresponds to the coefficient of Â(z/γ), sqrt( )corresponds to the square root operation and the tables exp_tab_p andexp_tab_q of size 34 contain the real and imaginary parts of the complexexponentials associated with the frequency of 6000 Hz, with

${{exp\_ tab}{{\_ p}\lbrack i\rbrack}} = \left\{ {{\begin{matrix}{\cos \left( {2\pi \frac{6000}{12800}i} \right)} & {{i = 0},\ldots \mspace{14mu},16} \\{- {\sin \left( {2\pi \frac{6000}{12800}\left( {33 - i} \right)} \right)}} & {{i = 17},\ldots \mspace{14mu},33}\end{matrix}{exp\_ tab}{{\_ q}\lbrack i\rbrack}} = \left\{ \begin{matrix}{\cos \left( {2\pi \frac{6000}{16000}i} \right)} & {{i = 0},\ldots \mspace{14mu},16} \\{- {\sin \left( {2\pi \frac{6000}{16000}\left( {33 - i} \right)} \right)}} & {{i = 17},\ldots \mspace{14mu},33}\end{matrix} \right.} \right.$

The additional prediction filter is obtained for example by suitablytruncating the polynomial Â(z) to the order 2.

In fact, the direct truncation to the order leads to the filter 1+â₁+â₂,which can pose a problem because there is generally nothing to guaranteethat this filter of order 2 is stable. In a preferred embodiment, thestability of the filter 1+â₁+â₂ is therefore detected and a filter1+â₁′+â₂′ is used, the coefficients of which are drawn from 1+â₁+â₂ as afunction of the instability detection. More specifically, the followingare initialized:

â _(i) ′=â _(i) ,i=1,2

The stability of the filter 1+â₁+â₂ can be verified differently; here, aconversion is used in the PARCOR coefficients (or reflectioncoefficients) domain by computing:

k ₁ =â ₁′/(1+â ₂′)

k ₂ =â ₂′

The stability is verified if |k_(i)|<1, i=1, 2. The value of k_(i) istherefore conditionally modified before ensuring the stability of thefilter, with the following steps:

$\left. k_{2}\leftarrow\left\{ {\begin{matrix}{\min \left( {0.6,k_{2}} \right)} & {k_{2} > 0} \\{\max \left( {{- 0.6},k_{2}} \right)} & {k_{2} < 0}\end{matrix}k_{1}}\leftarrow\left\{ \begin{matrix}{\min \left( {0.99,k_{2}} \right)} & {k_{1} > 0} \\{\max \left( {{- 0.99},k_{2}} \right)} & {k_{1} < 0}\end{matrix} \right. \right. \right.$

in which min(.,.) and max(.,.) respectively give the minimum and themaximum of 2 operands. It should be noted that the threshold values,0.99 for k₁ and 0.6 for k₂, will be able to be adjusted in variants ofthe invention. It will be recalled that the first reflectioncoefficient, k₁, characterizes the spectral slope (or tilt) of thesignal modeled to the order 1; in the invention the value of k₁ issaturated at a value close to the stability limit, in order to preservethis slope and retain a tilt similar to that of 1/Â(z). It will also berecalled that the second reflection coefficient, k₂, characterizes theresonance level of the signal modeled to the order 2; since the use of afilter of order 2 aims to eliminate the influence of such resonancesaround the frequency of 6000 Hz, the value of k₂ is more stronglylimited; this limit is set at 0.6.

The coefficients of 1+â₁′+â₂′ are then obtained by:

â ₁′=(1+k ₂)k ₁

â ₂ ′=k ₂

The frequency response of the additional filter is therefore finallycomputed:

$Q = \frac{1}{{\sum\limits_{k = 0}^{2}\; {{\hat{a}}_{k}^{\prime}^{{- j}\; k\; \theta}}}}$

with

$\theta = {2\pi {\frac{6000}{12800}.}}$

This quantity is computed preferentially according to the followingpseudo-code:

  qx = qy = 0 for 1 = 0 to 2  qx = qx + As[i]*exp_tab_q[i];  qy = qy +As[i]*exp_tab_q[33-i]; end for Q = 1/sqrt(qx*qx + qy*qy)in which As[i]=â_(i)′.

With no loss of generality, it will be possible to compute thecoefficients of the filter of order 2 otherwise, for example by applyingto the LPC filter Â(z) of order 16 the reduction procedure of the LPCorder called “STEP DOWN” described in J. D. Markel and A. H. Gray,Linear Prediction of Speech, Springer Verlag, 1976 or by performing twoLevinson-Durbin (or STEP-UP) algorithm iterations from theself-correlations computed on the signal synthesized (decoded) at 12.8kHz and windowed.

For some signals, the quantity Q, computed from the first 3 LPCcoefficients decoded, better takes account of the influence of thespectral slope (or tilt) in the spectrum and avoids the influence of“spurious” peaks or troughs close to 6000 Hz which can skew or raise thevalue of the quantity R, computed from all the LPC coefficients.

In a preferred embodiment, the optimized scale factor is deduced fromthe pre-computed quantities R, P, Q conditionally, as follows:

If the tilt (computed as in AMR-WB in the block 104, by normalizedself-correlation in the form r(1)/r(0) in which r(i) is theself-correlation) is negative (tilt <0 as represented in FIG. 5b ), thecomputation of the scale factor is done as follows:

-   -   to avoid artifacts due to excessively abrupt variations of        energy of the high band, a smoothing is applied to the value        of R. In a preferred embodiment, an exponential smoothing is        performed with a fixed factor in time (0.5) in the form of:

R=0.5R+0.5R _(prev)

R _(prev) =R

in which R_(prev) corresponds to the value of R in the precedingsubframe and the factor 0.5 is optimized empirically—obviously, thefactor 0.5 will be able to be changed for another value and othersmoothing methods are also possible. It should be noted that thesmoothing makes it possible to reduce the temporal variants andtherefore avoid artifacts.

The optimized scale factor is then given by:

g _(HB2)(m)=max(min(R,Q),P)/P

In an alternative embodiment, it will be possible to replace thesmoothing of R with a smoothing of g_(HB2)(m) such that:

g _(HB2)(m)←0.5g _(HB2)(m)+0.5g _(HB2)(m−1)

If the tilt (computed as in AMR-WB in the block 104) is positive(tilt >0 as in FIG. 5a ), the computation of the scale factor is done asfollows:

-   -   the quantity R is smoothed adaptively in time, with a stronger        smoothing when R is low—as in the preceding case, this smoothing        makes it possible to reduce the temporal variants and therefore        avoids artifacts:

R=(1−α)R+αR _(prev) with α=1−R ²

R _(prev) =R

Then, the optimized scale factor is given by:

g _(HB2)(m)=min(R,P,Q)/P

In an alternative embodiment, it will be possible to replace thesmoothing of R with a smoothing of g_(HB2)(m) as computed above.

g _(HB)(m)=(1−α)g _(HB)(m)+αg _(HB)(m−1),m=0, . . . ,3,α=1−g _(HB) ²(m)

where g_(HB)(−1) is the scale or gain factor computed for the lastsubframe of the preceding frame.

The minimum of R, P, Q is taken here in order to avoid overestimatingthe scale factor.

In a variant, the above condition depending only on the tilt will beable to be extended to take account not only of the tilt parameter butalso of other parameters in order to refine the decision. Furthermore,the computation of g_(HB2)(m) will be able to be adjusted according tothese said additional parameters.

An example of additional parameter is the number of zero crossings (ZCR,zero crossing rate) which can be defined as:

${zcr}_{s} = {\frac{1}{2}{\sum\limits_{n = 1}^{N - 1}\; {{{{sgn}\left\lbrack {s(n)} \right\rbrack} - {{sgn}\left\lbrack {s\left( {n - 1} \right)} \right\rbrack}}}}}$

in which

${{sgn}(x)} = \left\{ \begin{matrix}1 & {{{if}\mspace{14mu} x} \geq 0} \\{- 1} & {{{if}\mspace{14mu} x} < 0}\end{matrix} \right.$

The parameter zcr generally gives results similar to the tilt. A goodclassification criterion is the ratio between zcr_(s) computed for thesynthesized signal s(n) and zcr_(u) computed for the excitation signalu(n) at 12 800 Hz. This ratio is between 0 and 1, where 0 means that thesignal has a decreasing spectrum, 1 that the spectrum is increasing(which corresponds to (1−tilt)/2. In this case, a ratiozcr_(s)/zcr_(u)>0.5 corresponds to the case tilt <0, a ratiozcr_(s)/zcr_(u)<0.5 corresponds to tilt >0.

In a variant, it will be possible to use a function of a parametertilt_(hp) where tilt_(hp) is the tilt computed for the synthesizedsignal s(n) filtered by a high-pass filter with a cut-off frequency forexample at 4800 Hz; in this case, the response 1/Â(z/γ) from 6 to 8 kHz(applied at 16 kHz) corresponds to the weighted response of 1/Â(z) from4.8 to 6.4 kHz. Since 1/Â(z/γ) has a more flattened response, it isnecessary to compensate this change of tilt. The scale factor functionaccording to tilt_(hp) is then given in an embodiment by:(1−tilt_(hp))²+0.6. Q and R are therefore multiplied by min (1,(1−tilt_(hp))²+0.6 when tilt >0 or by max (1, (1−tilt_(hp))²+0.6) whentilt <0.

The case of the 23.85 kbit/s bit rate is now considered, for which again correction is performed by the blocks 403 to 408. This gaincorrection could moreover be the subject of a separate invention. Inthis particular embodiment according to the invention, the gaincorrection information, denoted g_(HBcorr)(m), transmitted by the AMR-WB(compatible) coding with a bit rate of 0.8 kbit/s, is used to improvethe quality at 23.85 kbit/s.

It is assumed here that the AMR-WB (compatible) coding has performed acorrection gain quantization on 4 bits as described in ITU-T clauseG.722.2/5.11 or, equivalently, in the 3GPP clause TS 26.190/5.11.

In the AMR-WB coder, the correction gain is computed by comparing theenergy of the original signal sampled at 16 kHz and filtered by a 6-7kHz bandpass filter, s_(HB)(n) with the energy of the white noise at 16kHz filtered by a synthesis filter 1/Â(z/γ) and a 6-7 kHz bandpassfilter (before the filtering, the energy of the noise is set to a levelsimilar to that of the excitation at 12.8 kHz), S_(HB2)(n). The gain isthe root of the ratio of energy of the original signal to the energy ofthe noise divided by two. In one possible embodiment, it will bepossible to change the bandpass filter for a filter with a wider band(for example from 6 to 7.6 kHz).

${{g_{HBcorr}(m)} = \sqrt{\frac{\sum\limits_{n = {80m}}^{{80{({m + 1})}} - 1}\; {s_{HB}(n)}^{2}}{\sum\limits_{n = {80m}}^{{80{({m + 1})}} - 1}{s_{{HB}\; 2}(n)}^{2}}}},{m = 0},\ldots \mspace{14mu},3$

To be able to apply the gain information received at 23.85 kbit/s (inthe block 407), it is important to bring the excitation to a levelsimilar to that expected of the AMR-WB (compatible) coding. Thus, theblock 404 performs the scaling of the excitation signal according to thefollowing equation:

u _(HB1)(n)=g _(HB3)(m)u _(HB)(n),n=80m, . . . ,80(m+1)−1

in which g_(HB3)(m) is a gain per subframe computed in the block 403 inthe form:

${g_{{HB}\; 3}(m)} = \sqrt{\frac{\sum\limits_{n = 0}^{63}\; {u(n)}^{2}}{5.{\sum\limits_{n = 0}^{79}{u_{HB}(n)}^{2}}}}$

in which the factor 5 in the denominator serves to compensate thebandwidth difference between the signal u(n) and the signal u_(HB)(n),given that, in the AMR-WB coding, the HF excitation is a white noiseover the 0-8000 Hz band.

The index of 4 bits per subframe, denoted index_(HF) _(_) _(gain)(m),sent at 23.85 kbit/s is demultiplexed from the bit stream (block 405)and decoded by the block 406 as follows:

g _(HBcorr)(m)=2·HP_gain(index_(HF) _(_) _(gain)(m))

in which HP_gain(.) is the HF gain quantization dictionary defined inthe AMR-WB coding and recalled below:

TABLE 1 (gain dictionary at 23.85 kbit/s) HP_gain(i) i 00.110595703125000 1 0.142608642578125 2 0.170806884765625 30.197723388671875 4 0.226593017578125 5 0.255676269531250 60.284545898437500 7 0.313232421875000 I 8 0.342102050781250 90.372497558593750 10 0.408660888671875 11 0.453002929687500 120.511779785156250 13  0.599822998046875f 14 0.741241455078125 150.998779296875000

The block 407 performs the scaling of the excitation signal according tothe following equation:

u _(HB2)(n)g _(HBcorr)(m)u _(HB1)(n),n=80m, . . . ,80(m+1)−1

Finally, the energy of the excitation is adjusted to the level of thecurrent subframe with the following conditions (block 408). Thefollowing is computed:

${{fac}(m)} = \sqrt{\frac{\sum\limits_{n = 0}^{79}\; \left( {{g(m)}{g_{{HB}\; 2}(m)}{u_{HB}(n)}} \right)^{2}}{\sum\limits_{n = 0}^{79}{u_{{HB}\; 2}(n)}^{2}}}$

The numerator here represents the high-band signal energy which would beobtained in the mode 23.05. As explained before, for the bit rates<23.85 kbit/s, it is necessary to retain the 3.0 level of energy betweenthe decoded excitation signal and the extended excitation signalu_(HB)(n), but this constraint is not necessary in the case of the 23.85kbit/s bit rate, since u_(HB)(n) is in this case scaled by the gain gH_(B3)(m). To avoid double multiplications, certain multiplicationoperations applied to the signal in the block 400 are applied in theblock 402 by multiplying by g(m). The value of g(m) depends on theu_(HB)(n) synthesis algorithm and must be adjusted such that the energylevel between the decoded excitation signal in low band and the signalg(m)u_(HB)(n) is retained.

In a particular embodiment, which will be described in detail later withreference to FIG. 7, g(m)=0.6g_(HB1)(m), where g_(HB1)(m) is a gainwhich ensures, for the signal u_(HB), the same ratio between energy persubframe and energy per frame as for the signal u(n) and 0.6 correspondsto the average frequency response amplitude value of the de-emphasisfilter from 5000 to 6400 Hz.

It is assumed that, in the block 408, there is information on the tiltof the low-band signal in a preferred embodiment, this tilt is computedas in the AMR-WB codec according to the blocks 103 and 104, but othermethods for estimating the tilt are possible without changing theprinciple of the invention.

If fac(m)>1 or tilt <0, the following is assumed:

u _(HB)′(n)=_(HB2)(n),n=80m, . . . ,80(m+1)−1

Otherwise:

u _(HB)′(n)=max(√{square root over (1−tilt)},fac(m))·u _(HB2)(n),n=80m,. . . ,80(m+1)−1

It will be noted that the optimized scale factor computation describedhere, notably in the blocks 401 and 402, is distinguished from theabovementioned equalization of filter levels performed in the AMR-WB+codec by a number of aspects:

-   -   The optimized scale factor is computed directly from the        transfer functions of the LPC filters without involving any        temporal filtering. This simplifies the method.    -   The equalization is preferably done at a frequency different        from the Nyquist frequency (6400 Hz) associated with the low        band. Indeed, the LPC modeling implicitly represents the        attenuation of the signal typically caused by the resampling        operations and therefore the frequency response of an LPC filter        may be subject at the Nyquist frequency to a decrease which is        not to the chosen common frequency.    -   The equalization here relies on a filter of lower order (here of        order 2) in addition to the 2 filters to be equalized. This        additional filter makes it possible to avoid the effects of        local spectral fluctuations (peaks or troughs) which may be        present at the common frequency for the computation of the        frequency response of the prediction filters.

For the blocks 403 to 408, the advantage of the invention is that thequality of the signal decoded at 23.85 kbit/s according to the inventionis improved relative to a signal decoded at 23.05 kbit/s, which is notthe case in an AMR-WB decoder. In fact, this aspect of the inventionmakes it possible to use the additional information (0.8 kbit/s)received at 23.85 kbit/s, but in a controlled manner (block 408), toimprove the quality of the extended excitation signal at the bit rate of23.85.

The device for determining the optimized scale factor as illustrated bythe blocks 401 to 408 of FIG. 4 implements a method for determining theoptimized scale factor now described with reference to FIG. 6.

The main steps are implemented by the block 401.

Thus, an extended excitation signal u_(HB)(n) is obtained in a frequencyband extension method E601 which comprises a step of decoding or ofextraction, in a first frequency band called low band, of an excitationsignal and of parameters of the first frequency band such as, forexample, the coefficients of the linear prediction filter of the firstfrequency band.

A step E602 determines a linear prediction filter called additionalfilter, of lower order 3.0 than that of the first frequency band. Todetermine this filter, the parameters of the first frequency banddecoded or extracted are used.

In one embodiment, this step is performed by truncation of the transferfunction of the linear prediction filter of the low band to obtain alower filter order, for example 2. These coefficients can then bemodified as a function of a stability criterion as explained previouslywith reference to FIG. 4.

From the coefficients of the additional filter thus determined, a stepE603 is implemented to compute the optimized scale factor to be appliedto the extended excitation signal. This optimized scale factor is, forexample, computed from the frequency response of the additional filterat a common frequency between the low band (first frequency band) andthe high band (second frequency band). A minimum value can be chosenbetween the frequency response of this filter and those of the low-bandand high-band filters.

This therefore avoids the overestimations of energy which could exist inthe methods of the prior art.

This step of computation of the optimized scale factor is, for example,described previously with reference to FIG. 4 and FIGS. 5a and 5 b.

The step E604 performed by the block 402 or 409 (depending on thedecoding bit rate) for the band extension, applies the duly computedoptimized scale factor to the extended excitation signal so as to obtainan optimized extended excitation signal u_(HB)′(n).

In a particular embodiment, the device for determining the optimizedscale factor 708 is incorporated in a band extension device nowdescribed with reference to FIG. 7. This device for determining theoptimized scale factor illustrated by the block 708 implements themethod for determining the optimized scale factor described previouslywith reference to FIG. 6.

In this embodiment, the band extension block 400 of FIG. 4 comprises theblocks 700 to 707 of FIG. 7 that is now described.

Thus, at the input of the band extension device, a low-band excitationsignal decoded or estimated by analysis is received (u(n)). The bandextension here uses the excitation decoded at 12.8 kHz (exc2 or u(n)) atthe output of the block 302 of FIG. 3.

It will be noted that, in this embodiment, the generation of theoversampled and extended excitation is performed in a frequency bandranging from 5 to 8 kHz therefore including a second frequency band(6.4-8 kHz) above the first frequency band (0-6.4 kHz).

Thus, the generation of an extended excitation signal is performed atleast over the second frequency band but also over a part of the firstfrequency band.

Obviously, the values defining these frequency bands can be differentdepending on the decoder or the processing device in which the inventionis applied.

For this exemplary embodiment, this signal is transformed to obtain anexcitation signal spectrum U(k) by the time-frequency transformationmodule 500.

In a particular embodiment, the transform uses a DCT-IV (for “DiscreteCosine Transform” type IV) (block 700) on the current frame of 20 ms(256 samples), without windowing, which amounts to directly transformingu(n) with n=0, . . . , 255 according to the following formula:

${U(k)} = {\sum\limits_{n = 0}^{N - 1}\; {{u(n)}{\cos \left( {\frac{\pi}{N}\left( {n + \frac{1}{2}} \right)\left( {k + \frac{1}{2}} \right)} \right)}}}$

in which N=256 and k=0, . . . , 255.

It should be noted here that the transformation without windowing (or,equivalently, with an implicit rectangular window of the length of theframe) is possible because the processing is performed in the excitationdomain, and not the signal domain so that no artifact (block effects) isaudible, which constitutes an important advantage of this embodiment ofthe invention.

In this embodiment, the DCT-IV transformation is implemented by FFTaccording to the so-called “Evolved DCT(EDCT)” algorithm described inthe article by D. M. Zhang, H. T. Li, A Low Complexity Transform—EvolvedDCT, IEEE 14th International Conference on Computational Science andEngineering (CSE), August 2011, pp. 144-149, and implemented in theITU-T standards G.718 Annex B and G.729.1 Annex E.

In variants of the invention, and without loss of generality, the DCT-IVtransformation will be able to be replaced by other short-termtime-frequency transformations of the same length and in the excitationdomain, such as an FFT (for “Fast Fourier Transform”) or a DCT-II(Discrete Cosine Transform type II). Alternatively, it will be possibleto replace the DCT-IV on the frame by a transformation withoverlap-addition and windowing of length greater than the length of thecurrent frame, for example by using an MDCT (for “Modified DiscreteCosine Transform”). In this case, the delay T in the block 310 of FIG. 3will have to be adjusted (reduced) appropriately as a function of theadditional delay due to the analysis/synthesis by this transform.

The DCT spectrum, U(k), of 256 samples covering the 0-6400 Hz band (at12.8 kHz), is then extended (block 701) into a spectrum of 320 samplescovering the 0-8000 Hz band (at 16 kHz) in the following form:

${U_{{HB}\; 1}(k)} = \left\{ \begin{matrix}0 & {{k = 0},\ldots \mspace{14mu},199} \\{U(k)} & {{k = 200},\ldots \mspace{14mu},239} \\{U\left( {k + {start\_ band} - 240} \right)} & {{k = 240},\ldots \mspace{14mu},319}\end{matrix} \right.$

in which it is preferentially taken that start_band=160.

The block 701 operates as module for generating an oversampled andextended excitation signal and performs a resampling from 12.8 to 16 kHzin the frequency domain, by adding ¼ of samples (k=240, . . . , 319) tothe spectrum, the ratio between 16 and 12.8 being 5/4.

Furthermore, the block 701 performs an implicit high-pass filtering inthe 0-5000 Hz band since the first 200 samples of U_(HB1)(k) are set tozero; as explained later, this high-pass filtering is also complementedby a part of progressive attenuation of the spectral values of indicesk=200, . . . , 255 in the 5000-6400 Hz band; this progressiveattenuation is implemented in the block 704 but could be performedseparately outside of the block 704. Equivalently, and in variants ofthe invention, the implementation of the high-pass filtering separatedinto blocks of coefficients of index k=0, . . . , 199 set to zero, ofattenuated coefficients k=200, . . . , 255 in the transformed domain,will therefore be able to be performed in a single step.

In this exemplary embodiment and according to the definition ofU_(HB1)(k), it will be noted that the 5000-6000 Hz band of U_(HB1)(k)(which corresponds to the indices k=200, . . . , 239) is copied from the5000-6000 Hz band of U(k). This approach makes it possible to retain theoriginal spectrum in this band and avoids introducing distortions in the5000-6000 Hz band upon the addition of the HF synthesis with the LFsynthesis—in particular the phase of the signal (implicitly representedin the DCT-IV domain) in this band is preserved.

The 6000-8000 Hz band of U_(HB1)(k) is here defined by copying the4000-6000 Hz band of U(k) since the value of start_band ispreferentially set at 160.

In a variant of the embodiment, the value of start_band will be able tobe made adaptive around the value of 160. The details of the adaptationof the start_band value are not described here because they go beyondthe framework of the invention without changing its scope.

For certain wide-band signals (sampled at 16 kHz), the high band (>6kHz) may be noisy, harmonic or comprise a mixture of noise andharmonics. Furthermore, the level of harmonicity in the 6000-8000 Hzband is generally correlated with that of the lower frequency bands.Thus, the noise generation block 702 performs a noise generation in thefrequency domain, U_(HBN)(k) for k=240, . . . , 319 (80 samples)corresponding to a second frequency band called high frequency in orderto then combine this noise with the spectrum U_(HB1)(k) in the block703.

In a particular embodiment, the noise (in the 6000-8000 Hz band) isgenerated pseudo-randomly with a linear congruential generator on 16bits:

${U_{HBN}(k)} = \left\{ \begin{matrix}0 & {{k = 0},\ldots \mspace{14mu},239} \\{{31821\mspace{14mu} {U_{HBN}\left( {k - 1} \right)}} + 13849} & {{k = 240},\ldots \mspace{14mu},319}\end{matrix} \right.$

with the convention that U_(HBN) (239) in the current frame correspondsto the value U_(HBN) (319) of the preceding frame. In variants of theinvention, it will be possible to replace this noise generation by othermethods.

The combination block 703 can be produced in different ways.Preferentially, an adaptive additive mixing of the following form isconsidered:

U _(HB2)(k)=βU _(HB1)(k)+αG _(HBN) U _(HBN)(k),k=240, . . . ,319

in which G_(HBN) is a normalization factor serving to equalize the levelof energy between the two signals,

$G_{HBN} = \sqrt{\frac{{\sum\limits_{k = 240}^{319}\; {U_{{HB}\; 1}(k)}^{2}} + ɛ}{{\sum\limits_{k = 240}^{319}\; {U_{{HB}\; N}(k)}^{2}} + ɛ}}$

with ε=0.01, and the coefficient α (between 0 and 1) is adjusted as afunction of parameters estimated from the decoded low band and thecoefficient β (between 0 and 1) depends on α.

In a preferred embodiment, the energy of the noise is computed in threebands: 2000-4000 Hz, 4000-6000 Hz and 6000-8000 Hz, with

$E_{{N\; 2} - 4} = {\sum\limits_{k \in {N{({80,159})}}}{U^{\prime 2}(k)}}$$E_{{N\; 4} - 6} = {\sum\limits_{k \in {N{({160,239})}}}{U^{\prime 2}(k)}}$$E_{{N\; 4} - 6} = {\sum\limits_{k \in {N{({240,319})}}}{U^{\prime 2}(k)}}$

in which

${U^{\prime}(k)} = \left\{ \begin{matrix}\sqrt{\frac{\sum\limits_{k = 160}^{239}\; {U^{2}(k)}}{\sum\limits_{k = 80}^{159}\; {U^{2}(k)}}{U(k)}} & {{k = 80},\ldots \mspace{14mu},159} \\{U(k)} & {{k = 160},\ldots \mspace{14mu},239} \\{\sqrt{\frac{\sum\limits_{k = 160}^{239}\; {U^{2}(k)}}{\sum\limits_{k = 240}^{319}\; {U_{{HB}\; 1}^{2}(k)}}}{U_{{HB}\; 1}(k)}} & {{k = 240},\ldots \mspace{14mu},319}\end{matrix} \right.$

and N(k₁,k₂) is the set of the indices k for which the coefficient ofindex k is classified as being associated with the noise. This set can,for example be obtained by detecting the local peaks in U′(k) thatverify |U′(k)|≧|U′(k−1)| and |U′(k)|≧|U′(k−1)| and by considering thatthese rays are not associated with the noise, i.e. (by applying thenegation of the preceding condition):

N(a,b)={a≦k≦b∥U′(k)|<|U′(k−1)| or |U′(k)|<|U′(k+1)|}

It can be noted that other methods for computing the energy of the noiseare possible, for example by taking the median value of the spectrum onthe band considered or by applying a smoothing to each frequency raybefore computing the energy per band.

α is set such that the ratio between the energy of the noise in the 4-6kHz and 6-8 kHz bands is the same as between the 2-4 kHz and 4-6 kHzbands:

$\alpha = \sqrt{\frac{\rho - E_{{N\; 6} - 8}}{{\sum\limits_{k = 160}^{239}\; {U^{2}(k)}} - E_{{N\; 6} - 8}}}$

in which

${E_{{N\; 4} - 6} = {\max \left( {E_{{N\; 4} - 6},E_{{N\; 2} - 4}} \right)}},{\rho = \frac{E_{{N\; 4} - 6}^{2}}{E_{{N\; 2} - 4}}},{\rho = {\max \left( {\rho,E_{{N\; 6} - 8}} \right)}}$

In variants of the invention, the computation of α will be able to bereplaced by other methods. For example, in a variant, it will bepossible to extract (compute) different parameters (or “features”)characterizing the signal in low band, including a “tilt” parametersimilar to that computed in the AMR-WB codec, and the factor α will beestimated as a function of a linear regression from these differentparameters by limiting its value between 0 and 1. The linear regressionwill, for example, be able to be estimated in a supervised manner byestimating the factor α by exchanging the original high band in alearning base. It will be noted that the way in which α is computed doesnot limit the nature of the invention.

In a preferred embodiment, the following is taken

β=√{square root over (1−α²)}

in order to preserve the energy of the extended signal after mixing.

In a variant, the factors β and α will be able to be adapted to takeaccount of the fact that a noise injected into a given band of thesignal is generally perceived as stronger than a harmonic signal withthe same energy in the same band. Thus, it will be possible to modifythe factors β and α as follows:

β←β·f(α)

α←α·f(α)

in which f(α) is a decreasing function of α, for examplef(α)=b−a√{square root over (α)}, b=1.1, a=1.2, f(α) limited from 0.3to 1. It must be noted that, after multiplication by f(α), α²+β²<1 sothat the energy of the signal U_(HB2)(k)=βU_(HB1)(k)+αG_(HBN)U_(HBN)(k)is lower than the energy of U_(HB1)(k) (the energy difference depends ona, the more noise is added, the more the energy is attenuated).

In other variants of the invention, it will be possible to take:

β=1−α

which makes it possible to preserve the amplitude level (when thecombined signals are of the same sign); however, this variant has thedisadvantage of resulting in an overall energy (at the level ofU_(HB2)(k)) which is not monotonous as a function of α.

It should therefore be noted here that the block 703 performs theequivalent of the block 101 of FIG. 1 to normalize the white noise as afunction of an excitation which is, by contrast here, in the frequencydomain, already extended to the rate of 16 kHz; furthermore, the mixingis limited to the 6000-8000 Hz band.

In a simple variant, it is possible to consider an implementation of theblock 703, in which the spectra, U_(HB1)(k) or G_(HBN)U_(HBN)(k), areselected (switched) adaptively, which amounts to allow only the values 0or 1 for α; this approach amounts to classifying the type of excitationto be generated in the 6000-8000 Hz band.

The block 704 optionally performs a double operation of application ofbandpass filter frequency response and of de-emphasis filtering in thefrequency domain.

In a variant of the invention, the de-emphasis filtering will be able tobe performed in the time domain, after the block 705, even before theblock 700; however, in this case, the bandpass filtering performed inthe block 704 may leave certain low-frequency components of very lowlevels which are amplified by de-emphasis, which can modify, in aslightly perceptible manner, the decoded low band. For this reason, itis preferred here to perform the de-emphasis in the frequency domain. Inthe preferred embodiment, the coefficients of index k=0, . . . , 199 areset to zero, so the de-emphasis is limited to the higher coefficients.

The excitation is first de-emphasized according to the followingequation:

${U_{{HB}\; 2}^{\prime}(k)} = \left\{ \begin{matrix}0 & {{k = 0},\ldots \mspace{14mu},199} \\{{G_{deemph}(k)}{U_{{HB}\; 2}(k)}} & {{k = 200},\ldots \mspace{14mu},255} \\{{G_{deemph}(255)}{U_{{HB}\; 2}(k)}} & {{k = 256},\ldots \mspace{14mu},319}\end{matrix} \right.$

in which G_(deemph)(k) is the frequency response of the filter1/(1−0.68z⁻¹) over a restricted discrete frequency band. By taking intoaccount the discrete (odd) frequencies of the DCT-IV, G_(deemph)(k) isdefined here as:

${{G_{deemph}(k)} = \frac{1}{{^{{j\theta}_{k}} - 0.68}}},{k = 0},\ldots \mspace{14mu},255$

in which

$\theta_{k} = {\frac{256 - 80 + k + \frac{1}{2}}{256}.}$

In the case where a transformation other than DCT-IV is used, thedefinition of θ_(k) will be able to be adjusted (for example for evenfrequencies).

It should be noted that the de-emphasis is applied in two phases fork=200, . . . , 255 corresponding to the 5000-6400 Hz frequency band,where the response 1/(1−0.68z⁻¹) is applied as at 12.8 kHz, and fork=256, . . . , 319 corresponding to the 6400-8000 Hz frequency band,where the response is extended from 16 kHz here to a constant value inthe 6.4-8 kHz 3.5 band.

It can be noted that, in the AMR-WB codec, the HF synthesis is notde-emphasized. In the embodiment presented here, the high frequencysignal is, on the contrary, de-emphasized so as to bring it into adomain consistent with the low frequency signal (0-6.4 kHz) which leavesthe block 305 of FIG. 3. This is important for the estimation and thesubsequent adjustment of the energy of the HF synthesis.

In a variant of the embodiment, in order to reduce the complexity, itwill be possible to set G_(deemph)(k) at a constant value independent ofk, by taking for example G_(deemph)(k)=0.6 which correspondsapproximately to the average value of G_(deemph)(k) for k=200, . . . ,319 in the conditions of the embodiment described above.

In another variant of the embodiment of the extension device, thede-emphasis will be able to be performed in an equivalent manner in thetime domain after inverse DCT.

In addition to the de-emphasis, a bandpass filtering is applied with twoseparate parts: one, high-pass, fixed, the other, low-pass, adaptive(function of the bit rate).

This filtering is performed in the frequency domain.

In the preferred embodiment, the low-pass filter partial response iscomputed in the frequency domain as follows:

${G_{lp}(k)} = {1 - {0.999\frac{k}{N_{lp} - 1}}}$

in which N_(Ip)=60 at 6.6 kbit/s, 40 at 8.85 kbit/s, and 20 at the bitrates >8.85 bit/s.

Then, a bandpass filter is applied in the form:

${U_{{HB}\; 3}(k)} = \left\{ \begin{matrix}0 & {{k = 0},\ldots \mspace{14mu},199} \\{{G_{hp}\left( {k - 200} \right)}{U_{{HB}\; 2}^{\prime}(k)}} & {{k = 200},\ldots \mspace{14mu},255} \\{U_{{HB}\; 2}^{\prime}(k)} & {{k = 256},\ldots \mspace{14mu},{319 - N_{lp}}} \\{{G_{lp}\left( {k - 320 - N_{lp}} \right)}{U_{{HB}\; 2}^{\prime}(k)}} & {{k = {320 - N_{lp}}},\ldots \mspace{14mu},319}\end{matrix} \right.$

The definition of G_(hp)(k), k=0, . . . , 55, is given, for example, intable 2 below.

TABLE 2 K g_(hp)(k) 0 0.001622428 1 0.004717458 2 0.008410494 30.012747280 4 0.017772424 5 0.023528982 6 0.030058032 7 0.037398264 80.045585564 9 0.054652620 10 0.064628539 11 0.075538482 12 0.08740332813 0.100239356 14 0.114057967 15 0.128865425 16 0.144662643 170.161445005 18 0.179202219 19 0.197918220 20 0.217571104 21 0.23813311422 0.259570657 23 0.281844373 24 0.304909235 25 0.328714699 260.353204886 27 0.378318805 28 0.403990611 29 0.430149896 30 0.45672201431 0.483628433 32 0.510787115 33 0.538112915 34 0.565518011 350.592912340 36 0.620204057 37 0.647300005 38 0.674106188 39 0.70052826040 0.726472003 41 0.751843820 42 0.776551214 43 0.800503267 440.823611104 45 0.845788355 46 0.866951597 47 0.887020781 48 0.90591964449 0.923576092 50 0.939922577 51 0.954896429 52 0.968440179 530.980501849 54 0.991035206 55 1.000000000

It will be noted that, in variants of the invention, the values ofG_(hP)(k) will be able to be modified while keeping a progressiveattenuation. Similarly, the low-pass filtering with variable bandwidth,G_(lp)(k), will be able to be adjusted with values or a frequency mediumthat are different, without changing the principle of this filteringstep.

It will also be noted that the bandpass filtering will be able to beadapted by defining a single filtering step combining the high-pass andlow-pass filtering.

In another embodiment, the bandpass filtering will be able to beperformed in an equivalent manner in the time domain (as in the block112 of FIG. 1) with different filter coefficients according to the bitrate, after an inverse DCT step. However, it will be noted that it isadvantageous to perform this step directly in the frequency domainbecause the filtering is performed in the domain of the LPC excitationand therefore the problems of circular convolution and of edge effectsare very limited in this domain.

It will also be noted that, in the case of the 23.85 kbit/s bit rate,the de-emphasis of the excitation U_(HB2)(k) is not performed to remainin agreement with the way in which the correction gain is computed inthe AMR-WB coder and to avoid double multiplications. In this case,block 704 performs only the low-pass filtering.

The inverse transform block 705 performs an inverse DCT on 320 samplesto find the high-frequency excitation sampled at 16 kHz. Itsimplementation is identical to the block 700, because the DCT-IV isorthonormal, except that the length of the transform is 320 instead of256, and the following is obtained:

${u_{{HB}\; 0}(n)} = {\sum\limits_{k = 0}^{N_{16k} - 1}\; {{U_{{HB}\; 3}(k)}{\cos \left( {\frac{\pi}{N_{16\; k}}\left( {k + \frac{1}{2}} \right)\left( {n + \frac{1}{2}} \right)} \right)}}}$

in which N_(16k)=320 and k=0, . . . , 319.

This excitation sampled at 16 kHz is then, optionally, scaled by gainsdefined per subframe of 80 samples (block 707).

In a preferred embodiment, a gain g_(HB1)(m) is first computed (block706) per subframe by energy ratios of the subframes such that, in eachsubframe of index m=0, 1, 2 or 3 of the current frame:

${g_{{HB}\; 1}(m)} = \sqrt{\frac{e_{3}(m)}{e_{2}(m)}}$

in which

${e_{1}(m)} = {{\sum\limits_{n = 0}^{63}\; {u\left( {n + {64\; m}} \right)}^{2}} + ɛ}$${e_{2}(m)} = {{\sum\limits_{n = 0}^{79}\; {u_{{HB}\; 0}\left( {n + {80\; m}} \right)}^{2}} + ɛ}$${e_{3}(m)} = {{e_{1}(m)}\frac{{\sum\limits_{n = 0}^{319}\; {u_{{HB}\; 0}(n)}^{2}} + ɛ}{{\sum\limits_{n = 0}^{255}\; {u(n)}^{2}} + ɛ}}$

with ε=0.01. The gain per subframe g_(HB1)(m) can be written in theform:

${g_{{HB}\; 1}(m)} = \sqrt{\frac{\frac{{\sum\limits_{n = 0}^{63}\; {u\left( {n + {64\; m}} \right)}^{2}} + ɛ}{{\sum\limits_{n = 0}^{255}\; {u(n)}^{2}} + ɛ}}{\frac{{\sum\limits_{n = 0}^{79}\; {u_{{HB}\; 0}\left( {n + {80\; m}} \right)}^{2}} + ɛ}{{\sum\limits_{n = 0}^{319}\; {u_{{HB}\; 0}(n)}^{2}} + ɛ}}}$

which shows that, in the signal u_(HB), the same ratio between energyper subframe and energy per frame as in the signal u(n) is assured.

The block 707 performs the scaling of the combined signal according tothe following equation:

u _(HB)(n)=g _(HB1)(m)u _(HB0)(n),n=80m, . . . ,80(m+1)−1

It will be noted that the implementation of the block 706 differs fromthat of the block 101 of FIG. 1, because the energy at the current framelevel is taken into account in addition to that of the subframe. Thismakes it possible to have the ratio of the energy of each subframe inrelation to the energy of the frame. The energy ratios (or relativeenergies) are therefore compared rather than the absolute energiesbetween low band and high band.

Thus, this scaling step makes it possible to retain, in the high band,the energy ratio between the subframe and the frame in the same way asin the low band.

It will be noted here that, in the case of the 23.85 kbit/s bit rate,the gains g_(HB1)(m) are computed but applied in the next step, asexplained with reference to FIG. 4, to avoid the double multiplications.In this case u_(HB)(n)=u_(HB0)(n).

According to the invention, the block 708 then performs a scale factorcomputation per subframe of the signal (steps E602 to E603 of FIG. 6),as described previously with reference to FIG. 6 and detailed in FIGS. 4and 5.

Finally, the corrected excitation u_(HB)′(n) is filtered by thefiltering module 710 which can be performed here by taking as transferfunction 1/Â(z/γ), in which γ=0.9 at 6.6 kbit/s and γ=0.6 at the otherbit rates, which limits the order of the filter to the order 16.

In a variant, this filtering will be able to be performed in the sameway as is described for the block 111 of FIG. 1 of the AMR-WB decoder,but the order of the filter changes to 20 at the 6.6 bit rate, whichdoes not significantly change the quality of the synthesized signal. Inanother variant, it will be possible to perform the LPC synthesisfiltering in the frequency domain, after having computed the frequencyresponse of the filter implemented in the block 710.

In a variant embodiment, the step of filtering by a linear predictionfilter 710 for the second frequency band is combined with theapplication of the optimized scale factor, which makes it possible toreduce the processing complexity. Thus, the steps of filtering 1/Â(z/γ)and of application of the optimized scale factor g_(HB2) are combined ina single step of filtering g_(HB2)/Â(z/γ) to reduce the processingcomplexity.

In variant embodiments of the invention, the coding of the low band(0-6.4 kHz) will be able to be replaced by a CELP coder other than thatused in AMR-WB, such as, for example, the CELP coder in G.718 at 8kbit/s. With no loss of generality, other wide-band coders or codersoperating at frequencies above 16 kHz, in which the coding of the lowband operates with an internal frequency at 12.8 kHz, could be used.Moreover, the invention can obviously be adapted to sampling frequenciesother than 12.8 kHz, when a low-frequency coder operates with a samplingfrequency lower than that of the original or reconstructed signal. Whenthe low-band decoding does not use linear prediction, there is noexcitation signal to be extended, in which case it will be possible toperform an LPC analysis of the signal reconstructed in the current frameand an LPC excitation will be computed so as to be able to apply theinvention.

Finally, in another variant of the invention, the excitation (u(n)) isresampled, for example by linear interpolation or cubic “spline”, from12.8 to 16 kHz before transformation (for example DCT-IV) of length 320.This variant has the defect of being more complex, because the transform(DCT-IV) of the excitation is then computed over a greater length andthe resampling is not performed in the transform domain.

Furthermore, in variants of the invention, all the computationsnecessary for the estimation of the gains (G_(HBN), g_(HB1)(m),g_(HB2)(m), g_(HBN), . . . ) will be able to be performed in alogarithmic domain.

In variants of the band extension, the excitation in low band u(n) andthe LPC filter 1/Â(z) will be estimated per frame, by LPC analysis of alow-band signal for which the band has to be extended. The low-bandexcitation signal is then extracted by analysis of the audio signal.

In a possible embodiment of this variant, the low-band audio signal isresampled before the step of extracting the excitation, so that theexcitation extracted from the audio signal (by linear prediction) isalready resampled.

The band extension illustrated in FIG. 7 is applied in this case to alow band which is not decoded but analyzed.

FIG. 8 represents an exemplary physical embodiment of a device fordetermining an optimized scale factor 800 according to the invention.The latter can form an integral part of an audio frequency signaldecoder or of an equipment item receiving audio frequency signals,decoded or not.

This type of device comprises a processor PROC cooperating with a memoryblock BM comprising a storage and/or working memory MEM.

Such a device comprises an input module E suitable for receiving anexcitation audio signal decoded or extracted in a first frequency bandcalled low band (u(n) or U(k)) and the parameters of a linear predictionsynthesis filter (Â(z)). It comprises an output module S suitable fortransmitting the synthesized and optimized high-frequency signal(u_(HB)′(n)) for example to a filtering module like the block 710 ofFIG. 7 or to a resampling module like the module 311 of FIG. 3.

The memory block can advantageously comprise a computer programcomprising code instructions for implementing the steps of the methodfor determining an optimized scale factor to be applied to an excitationsignal or to a filter within the meaning of the invention, when theseinstructions are executed by the processor PROC, and notably the stepsof determination (E602) of a linear prediction filter, called additionalfilter, of lower order than the linear prediction filter of the firstfrequency band, the coefficients of the additional filter being obtainedfrom parameters decoded or extracted from the first frequency band, andof computation (E603) of an optimized scale factor as a function atleast of the coefficients of the additional filter.

Typically, the description of FIG. 6 reprises the steps of an algorithmof such a computer program. The computer program can also be stored on amemory medium that can be read by a reader of the device or that can bedownloaded into the memory space thereof.

The memory MEM stores, generally, all the data necessary for theimplementation of the method.

In a possible embodiment, the device thus described can also comprisefunctions for application of the optimized scale factor to the extendedexcitation signal, of frequency band extension, of low-band decoding andother processing functions described for example in FIGS. 3 and 4 inaddition to the optimized scale factor determination functions accordingto the invention.

Although the present disclosure has been described with reference to oneor more examples, workers skilled in the art will recognize that changesmay be made in form and detail without departing from the scope of thedisclosure and/or the appended claims.

1. A band extension method comprising: receiving an excitation signal ina band extension device and performing the following acts by the bandextension device to determine an optimized scale factor to be applied toan excitation signal or to a filter in an audio frequency signalfrequency band extension method; decoding or of extraction, in a firstfrequency band, of the excitation signal and of parameters of the firstfrequency band comprising coefficients of a linear prediction filter;generation of an extended excitation signal on at least one secondfrequency band; filtering, by a linear prediction filter, for the secondfrequency band; determination of a linear prediction filter called anadditional filter, of lower order than the linear prediction filter ofthe first frequency band, coefficients of the additional filter beingobtained from the parameters decoded or extracted from the firstfrequency band; computation of the optimized scale factor as a functionat least of the coefficients of the additional filter.
 2. The method asclaimed in claim 1, wherein the band extension method comprisesapplication of the optimized scale factor to the extended excitationsignal.
 3. The method as claimed in claim 2, wherein the application ofthe optimized scale factor is combined with the act of filtering in thesecond frequency band.
 4. The method as claimed in claim 1, wherein thecoefficients of the additional filter are obtained by truncation of thetransfer function of the linear prediction filter of the first frequencyband to obtain a lower order.
 5. The method as claimed in claim 4,wherein the coefficients of the additional filter are modified as afunction of a stability criterion of the additional filter.
 6. Themethod as claimed in claim 1, wherein the computation of the optimizedscale factor comprises: computation of the frequency responses of thelinear prediction filters of the first and second frequency bands for acommon frequency; computation of the frequency response of theadditional filter for this common frequency; computation of theoptimized scale factor as a function of the duly computed frequencyresponses.
 7. The method as claimed in claim 1, wherein the methodfurther comprises the following acts, implemented for a predetermineddecoding bit rate: first scaling of the extended excitation signal by again computed for each subframe as a function of an energy ratio betweenthe decoded excitation signal and the extended excitation signal; secondscaling of the excitation signal obtained from the first scaling by adecoded correction gain; adjustment of the energy of the excitation forthe current subframe by an adjustment factor computed as a function ofthe energy of the signal obtained after the second scaling and as afunction of the signal obtained after application of the optimized scalefactor.
 8. A determination device for determining an optimized scalefactor to be applied to an excitation signal or to a filter in an audiofrequency signal frequency band extension device, the band extensiondevice comprising a module for decoding or extracting, in a firstfrequency band, an excitation signal and parameters of the firstfrequency band comprising coefficients of a linear prediction filter, amodule for generating an extended excitation signal on at least onesecond frequency band and a module for filtering, by a linear predictionfilter, for the second frequency band, the determination devicecomprising: an input receiving the excitation signal; a moduleconfigured to determine a linear prediction filter called an additionalfilter, of lower order than the linear prediction filter of the firstfrequency band, the coefficients of the additional filter being obtainedfrom the parameters decoded or extracted from the first frequency band;and a module configured to compute the optimized scale factor as afunction at least of the coefficients of the additional filter.
 9. Anaudio frequency signal decoder comprising the determination deviceaccording to claim
 8. 10. (canceled)
 11. A non-transitory storage mediumthat can be read by a device for determining an optimized scale factoron which is stored a computer program comprising code instructions forexecution of a method for determining the optimized scale factor whenthe code instructions are executed by a processor, wherein the methodcomprises: receiving an excitation signal in a band extension device andperforming the following acts by the band extension device to determinean optimized scale factor to be applied to an excitation signal or to afilter in an audio frequency signal frequency band extension method;decoding or of extraction, in a first frequency band, of the excitationsignal and of parameters of the first frequency band comprisingcoefficients of a linear prediction filter; generation of an extendedexcitation signal on at least one second frequency band; filtering, by alinear prediction filter, for the second frequency band; determinationof a linear prediction filter called an additional filter, of lowerorder than the linear prediction filter of the first frequency band,coefficients of the additional filter being obtained from the parametersdecoded or extracted from the first frequency band; computation of theoptimized scale factor as a function at least of the coefficients of theadditional filter.